˚
detector using Cu-Ka radiation (l 5 1.54178 A). The images were
interpreted and integrated with the program SAINT from Bruker,
between measurements) to a 12 mW UV-lamp (324 nm). This
photostability test was carried out in comparison with a solution in
acetonitrile and a sample of the latter without UV irradiation
15
C
42
H
35EuF12
N
2
O
8
S
4
, M 5 1203.92, monoclinic, P2 /c, a 5 12.4045(8),
1
3
˚
˚
21
b 5 18.6683(16), c 5 20.5603(14) A, b 5 97.167(5)u, V 5 4724.0(6) A ,
23
(except for excitation during measurements). The quantum yield of
c
T 5 100(2) K, Z 5 4, D 5 1.693 g cm , m(Cu-Ka) 5 12.060 mm ,
F(000) 5 2400, crystal size 0.5 6 0.2 6 0.1 mm, 8007 independent
reflections (Rint 5 0.1816). Final R 5 0.0843 for 4845 reflections with I .
the solution of 1 in the ionic liquid [HMIM][Tf N] stabilized at
2
about 98% of the initial value for the fresh sample—the slight
decay is probably due to traces of water in the ionic liquid, which
could be introduced by handling the sample and which quenches
2s(I) and wR2 5 0.2185 for all data. The structure was solved by direct
methods and refined by full-matrix least-squares on F using the
2
1
6
SHELXTL program package. Non-hydrogen atoms were anisotropically
refined and the hydrogen atoms in the riding mode with isotropic
temperature factors fixed at 1.2 times U(eq) of the parent atoms (1.5 times
for crystallographic data in CIF or other electronic format.
luminescence. The dry [HMIM][Tf N] ionic liquid is hygroscopic,
2
but due to the absence of vapour pressure water can efficiently be
removed.
In the ionic liquid [HMIM][Br], significant changes in the fine
§ The quantum yield measurements were performed by means of an
integrating sphere. The absolute error on the quantum yield values is about
¡0.5%. The tetrakis(2-thenoyltrifluoro-acetonato)europate(III) complex
was excited at a wavelength of 340 nm.
structure of the emission of [HMIM][Eu(tta)
7
4
] can be observed.
2
emission at 615 nm is a hypersensitive transition
5
The D
0
A F
that reveals changes of the coordination sphere of the
europium(III) ion. This can be seen in Fig. 3. Changes are also
indicated by the dramatic decrease of the quantum yield down to
1
M. H. V. Werts, R. H. Woudenberg, P. G. Emmerink, R. van Gassel,
J. W. Hofstraat and J. W. Verhoeven, Angew. Chem., Int. Ed., 2000, 39,
4542; A. Beeby, S. W. Botchway, I. M. Clarkson, S. Faulkner,
A. W. Parker, D. Parker and J. A. G. Williams, J. Photochem.
Photobiol., B, 2000, 57, 89; T. Yamada, S. Shinoda and H. Tsukube,
Chem. Commun., 2002, 1218.
14% for the fresh solution in the [HMIM][Br] ionic liquid,
compared to 61% in an acetonitrile solution. The most probable
explanation for this behaviour is a partial exchange of the
b-diketonate ligands by bromide anions, thus resulting in a less
efficient energy transfer.
2 J.-C. G. B u¨ nzli and G. R. Choppin, in Lanthanide Probes in Life,
Chemical and Earth Sciences – Theory and Practice, Elsevier,
Amsterdam, 1989; C. G o¨ rller-Walrand and K. Binnemans, in
Handbook on the Physics and Chemistry of Rare Earths, ed. K. A.
Gschneidner, Jr. and L. Eyring, North-Holland, Amsterdam, 1998,
vol. 25, ch. 167, p. 101.
The reason for the improved photochemical stabilization of
[
HMIM][Eu(tta) ] in the ionic liquid [HMIM][Tf
4
2
N] is still not
] leads to
understood, but the crystal structure of [HMIM][Eu(tta)
4
the assumption that hydrogen bonding between cation and ligands
could play a significant role, since it encapsulates the complex. A
strong interaction between host medium and guest is known to
remarkably influence the photophysical and photochemical
3 R. Reyes, M. Cremona, E. E. S. Teotonio, H. F. Brito and O. L. Malta,
Chem. Phys. Lett., 2004, 396, 54; J. Kido and Y. Okamoto, Chem. Rev.,
2002, 102, 2537; C. Adachi, M. A. Baldo and S. R. Forrest, J. Appl.
Phys., 2000, 87, 8049.
4 F. R. G. Silva, J. F. S. Menezes, G. B. Rocha, S. Alves, H. F. Brito,
R. L. Longo and O. L. Malta, J. Alloys Compd., 2000, 303–304, 364.
12
processes of a guest molecule. Therefore computational mole-
5
T. Pagnot, P. Audebert and G. Tribillon, Chem. Phys. Lett., 2000, 322,
572.
K. R. Seddon, J. Chem. Technol. Biotechnol., 1997, 68, 351; R. Sheldon,
Chem. Commun., 2001, 2399; T. Welton, Chem. Rev., 1999, 99, 2071;
J. S. Wilkes, Green Chem., 2002, 4, 73; P. Wasserscheid and W. Keim,
Angew. Chem., Int. Ed., 2000, 39, 3772.
cular modelling of the complex in an ionic liquid has to be
14
performed (similar to the studies by Chaumont et al.).
6
Nevertheless, along with the versatile properties of ionic liquids,
this system appears to have the potential to be developed to a new
class of luminescent ‘soft’ materials.
7
8
J. L. Anderson, J. Ding, T. Welton and D. W. Armstrong, J. Am.
Chem. Soc., 2002, 124, 14247; V. Znamenskiy and M. N. Kobrak,
J. Phys. Chem. B, 2004, 108, 1072; S. V. Dzyuba and R. A. Bartsch,
Tetrahedron Lett., 2002, 43, 4657; S. N. V. K. Aki, J. F. Brennecke and
A. Samanta, Chem. Commun., 2001, 413; A. J. Carmichael and
K. R. Seddon, J. Phys. Org. Chem., 2000, 13, 591.
K. Driesen, P. Nockemann and K. Binnemans, Chem. Phys. Lett., 2004,
395, 306; S. Arenz, A. Babai, K. Binnemans, K. Driesen, R. Giernoth,
A.-V. Mudring and P. Nockemann, Chem. Phys. Lett., 2005, 402, 75;
I. Billard, S. Mekki, C. Gaillard, P. Hesemann, G. Moutiers, C. Mariet,
A. Labet and J.-C. G. B u¨ nzli, Eur. J. Inorg. Chem., 2004, 6, 1190;
E. Guillet, D. Imbert, R. Scopelliti and J.-C. G. B u¨ nzli, Chem. Mater.,
In summary, we found that the 1-hexyl-3-methylimidazolium
tetrakis(2-thenoyltrifluoroacetonato)europate(III)
complex
is
photochemically stabilized in a weakly-coordinating imidazolium-
based ionic liquid. The tunable properties of ionic liquids together
with the stabilization of b-diketonate complexes can open up new
potential applications for these materials, e.g. as laser dyes or as
materials for emissive displays. Currently we expand our research
on the stability of tetrakis(b-diketonate) complexes in ionic liquids
3
+
towards other lanthanides emitting in the visible region like Tb
3+
and Sm , as well as towards the lanthanides emitting in the near-
3+
2
004, 16, 4063.
9 P. Kolle and R. Dronskowski, Inorg. Chem., 2004, 43, 2803.
0 Y. Hasegawa, K. Sogabe, Y. Wada and S. Yanagida, J. Lumin., 2003,
01, 235; R. Van Deun, P. Nockemann, C. G o¨ rller-Walrand and
K. Binnemans, Chem. Phys. Lett., 2004, 397, 447.
3
+
3+
infrared region (Er , Nd , Yb ). The preliminary results are very
promising.
1
1
KB, KD and RVD thank the F.W.O.-Flanders (Belgium) for a
Postdoctoral Fellowship. PN is a Postdoctoral Fellow funded by
the EU (GROWTH No: GRD2-2000-30346 OPAMD). Financial
support by the F.W.O.-Flanders (G.0117.03), by the K.U. Leuven
11 L. D. Carlos, C. De Mello Donega, R. Q. Albuquerque, S. Alves, Jr.,
J. F. S. Menezes and O. L. Malta, Mol. Phys., 2003, 101, 1037.
12 Q. Xu, L. Li, B. Li, J. Yu and R. Xu, Microporous Mesoporous Mater.,
2
000, 38, 351.
3 C. G. Gameiro, C. A. Achete, R. A. Sim a˜ o, E. F. da Silva, Jr. and
P. A. Santa-Cruz, J. Alloys Compd., 2002, 344, 385.
4 A. Chaumont and G. Wipff, Phys. Chem. Chem. Phys., 2003, 5, 3481.
(
GOA 03/03) and by the EU (GROWTH No: GRD2-2000-30346
1
OPAMD) is gratefully acknowledged.
1
1
5 SAINT, version 5/6.0, Bruker Analytical X-ray Systems Inc., Madison,
Notes and references
WI, 1997.
16 SHELXTL-PC, version 5.1, Bruker Analytical X-ray Systems Inc.,
Madison, WI, 1997.
{ Crystal data for compound 1: crystals were grown from ethanol, intensity
data were collected on a SMART 6000 diffractometer equipped with CCD
4
356 | Chem. Commun., 2005, 4354–4356
This journal is ß The Royal Society of Chemistry 2005